JPH0248966B2 - JIKIKIROKUTAI * SONOSEIZOHONARABINISEIZOSOCHI - Google Patents
JIKIKIROKUTAI * SONOSEIZOHONARABINISEIZOSOCHIInfo
- Publication number
- JPH0248966B2 JPH0248966B2 JP4933084A JP4933084A JPH0248966B2 JP H0248966 B2 JPH0248966 B2 JP H0248966B2 JP 4933084 A JP4933084 A JP 4933084A JP 4933084 A JP4933084 A JP 4933084A JP H0248966 B2 JPH0248966 B2 JP H0248966B2
- Authority
- JP
- Japan
- Prior art keywords
- film
- quasi
- magnetic
- magnetic recording
- perpendicularly magnetized
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Lifetime
Links
- 230000005291 magnetic effect Effects 0.000 claims description 44
- 230000005415 magnetization Effects 0.000 claims description 20
- 239000000758 substrate Substances 0.000 claims description 17
- 238000004519 manufacturing process Methods 0.000 claims description 12
- 239000000203 mixture Substances 0.000 claims description 10
- 239000000463 material Substances 0.000 claims description 7
- 229910052751 metal Inorganic materials 0.000 claims description 6
- 239000002184 metal Substances 0.000 claims description 6
- 239000000956 alloy Substances 0.000 claims description 5
- 229910045601 alloy Inorganic materials 0.000 claims description 5
- 238000001704 evaporation Methods 0.000 claims description 5
- 230000008020 evaporation Effects 0.000 claims description 5
- 230000002265 prevention Effects 0.000 claims description 4
- 238000010438 heat treatment Methods 0.000 claims description 2
- 239000002245 particle Substances 0.000 description 5
- 239000013078 crystal Substances 0.000 description 4
- 238000000151 deposition Methods 0.000 description 4
- 238000010586 diagram Methods 0.000 description 4
- 230000005294 ferromagnetic effect Effects 0.000 description 4
- 230000008021 deposition Effects 0.000 description 3
- 238000000034 method Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 2
- 238000005259 measurement Methods 0.000 description 2
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 238000005566 electron beam evaporation Methods 0.000 description 1
- 239000007789 gas Substances 0.000 description 1
- 238000007733 ion plating Methods 0.000 description 1
- 239000000696 magnetic material Substances 0.000 description 1
- 230000005389 magnetism Effects 0.000 description 1
- 150000002739 metals Chemical class 0.000 description 1
- 239000001301 oxygen Substances 0.000 description 1
- 229910052760 oxygen Inorganic materials 0.000 description 1
- 230000002093 peripheral effect Effects 0.000 description 1
- 230000000630 rising effect Effects 0.000 description 1
- 238000004544 sputter deposition Methods 0.000 description 1
- 238000001771 vacuum deposition Methods 0.000 description 1
- 238000004804 winding Methods 0.000 description 1
Landscapes
- Magnetic Record Carriers (AREA)
- Recording Or Reproducing By Magnetic Means (AREA)
- Manufacturing Of Magnetic Record Carriers (AREA)
Description
本発明は、リングヘツドを用いて記録を行なう
に適した磁気記録体、その製造法並にその製造装
置に関する。
従来の垂直磁化膜をもつ磁気記録体を用い、記
録するにリングヘツドで行なう場合は、第1図示
の如くリングヘツドが半円状の磁界を発生するた
め、垂直ヘツドに比べてその高密度記録特性と再
生出力が劣ると云う欠点を有する。即ち、リング
ヘツドでは、垂直磁化膜の膜表面側では垂直方向
の磁界成分が強いが、ヘツドから離れた側すなわ
ち膜の内部や基板との界面近傍では平行方向の磁
界成分が多くなる。このため、膜の内部や基板と
の界面近傍では充分磁化されなくなる。これは、
完全な垂直磁化膜では平行方向が困難磁化方向で
あるためである。
本発明は、この点を種々検討した結果、これを
改善し、完全な垂直磁化膜(Hc⊥/Hc>1、
Mr⊥/Mr>1)より面内方向にも高い保磁力
と残留磁束密度を発生するリングヘツドによる記
録、再生に優れた磁気記録体を提供するもので、
非磁性基板上に、下記の条件を満足している準垂
直磁化膜を備えることを特徴とする磁気記録体。
Hc⊥/Hc≧1 Hc≧400θe
1≧Mr⊥/Mr≧0.5
茲で、
Hc⊥:膜面に対して垂直方向の保磁力
Hc:膜面に対して平行方向で記録再生時の走
行方向の保磁力
Mr⊥:膜面に対して垂直方向の残留磁化
Mr:膜面に対して平行方向で記録再生時の走
行方向の残留磁化
上記本発明の磁気記録体をリングヘツドを用い
てその準垂直磁化膜を磁化した様子を第2図に示
す通りで、その膜aは、垂直方向に磁気異方性を
もつており垂直方向の保磁力も大きいので、垂直
方向の磁界成分が大きい膜表面近傍では従来の完
全な垂直磁化膜を用いる場合と同様に垂直に磁化
されていると共に膜内部や基板bとの界面近傍で
は、リングヘツドcの発生する半円状の磁界の水
平方向の磁界成分に沿つて磁化することになるの
で、膜内部や基板a2近傍との界面近傍での反磁界
が減少し、従つて、高い再生出力と高記録密度特
性を得ることができる。而して、本発明の準垂直
磁化膜は、リングヘツドの発生する磁界に沿つて
磁化されることが可能である。特に膜表面では垂
直方向に大きい反磁界が発生するので、Hc⊥/
Hc>1という条件が必要不可欠である。
上記磁気特性において、更に膜面内における磁
気異方性の方向が記録方向に一致しているもの
は、更に自己減磁作用を低減することができ、更
に高密度記録特性と再生出力を向上させることが
できる。この方向とは、磁気テープの場合は長さ
方向であり、デイスクの場合には円周方向であ
る。この準垂直磁化膜では、上記の特徴条件から
分るように膜全体の磁気異方性は垂直方向であり
更にその上で膜面における異方性が記録方向と一
致しているという磁気特性となつている。先に、
発明者等は、(Fe、Co、Ni)−O系の垂直磁化膜
を、Fe、Co、Niやこれらの合金をO2ガスが導入
された真空雰囲気中で、加熱しない非磁性基板面
にほとんど垂直に入射蒸着させることにより製造
する方法を提案したが、本発明は、上記の準垂直
磁化膜をこれと略同様の方法で作成可能であるこ
とが分つた。即ち、上記の製造法において、多
少、垂直磁気磁性で低下するようにすれば良く、
例えば非磁性基板を加熱し100〜400℃の範囲に保
持したものに同様のほとんど垂直蒸着を行なうこ
とにより得られることが分つた。即ち、加熱した
基板に、非強磁性酸化物微粒子と金属強磁性微粒
子の混合体が付着するとその熱により金属強磁性
微粒子の粗大化が起り保磁力が増加すると同時に
垂直配列が乱れてくるので垂直磁気異方性が減少
し、その結果、本発明の準垂直磁化膜となること
を知見した。400℃を大きくこえると粒子の大き
さが大きくなりすぎるため保磁力が減少する。準
垂直磁化膜の製法は、真空蒸着法、イオンプレー
テイング法、スパツタリング法のいづれにおいて
も可能である。
次に、本発明の上記準垂直磁化膜をもつ磁気記
録体の製造法の実施例をその代表的な製造装置と
共に第3図につき詳述する。1は真空ポンプに接
続される排気口2をもつ真空処理容器を示し、該
容器1内に加熱される回転金属性円胴体(キヤ
ン)3を中心に配し、その上方両側にテープ状非
磁性基材aの巻き解しローラー4と巻き取りロー
ラー5を設け、該テープ状非磁性基材bをこれら
4,5間にその中間の円胴体3の周面に添着させ
た状態で架け渡し、これを矢示の方向に所定速度
で走行させるようにした。該円胴体3の直下には
電子ビーム蒸発源6を設け、該円胴体3の下端面
近傍に少許の空隙7を存してその両側に防着板
8,9を配設し、その少くとも1方の防着板Aを
水平方向に、図面で左右に移動自在に設置し、蒸
発源6からのFe、Co、Niやこれらの合金から成
す材料bの蒸発原子が入射角θ1で蒸着されるよう
に適宜調節できるようにした。1方の防着板9と
の入射角θ2も必要に応じ同様に移動自在となし得
る。更に、この蒸発域内にO2が吹き出すように
開口するO2導入用管10を容器1壁に気密に貫
通して設ける。かゝる装置を使用し、次のように
作動せしめる。即ち、非磁性基板a2を矢示方向に
走行させ、任意の手段で内部から加熱された例え
ば300℃に加熱された円胴体3の外周面に接触さ
せてその基板bを300℃に加熱し、この加熱基板
a面にその円胴体3の下端面を通過する間に、そ
の空隙7を介して下方から上昇する強磁性金属蒸
発原子をほとんど垂直に入射角蒸着せしめ、その
準垂直磁化膜aの形成された後ローラー5に巻き
取るようにする。比較試験としてθ1を0゜と30゜の2
種類について行なつた。θ2は30゜一定とした。作
成された磁化膜の膜面内の磁気異方性はθ1が0゜の
場合は認められないが、θ1が30゜の場合は、テー
プ長手方向に面内の磁気異方性が発生した。これ
は、最初に基材面に発生する核の方向がその後の
結晶の成長方向を決定するためで、θ1が0゜の場合
には垂直に結晶が成長するに対して、θ1が30゜の
場合には長手方向に少し傾斜した結晶成長が行な
われるためと考えられる。1方、上記の加熱され
た基材の熱のため、粒子の粗大化がおこり、その
垂直方向の配列が崩れることにより、本発明の準
垂直磁化膜の生成が保証される。
以上の装置によりθ1=0゜にしてFe、Co、Ni及
びこれら合金の各種組成、及びこの各種金属とO
原子との配合組成を変えた各種の磁化膜を作成し
各種磁気特性を測定した。その結果を第4図乃至
第15図に示す。これらの結果から、本発明の前
記磁気特性条件をもつ準垂直磁化膜は、(FexCoy
Niz)1-nOnで表わされる組成において、0≦x≦
0.05、0≦z≦0.40(但しx+y+z=1)、0.10
≦m≦0.40の範囲のもの、及び上記組成におい
て、0.40≦x≦1.0、0≦z≦0.25(但しx+y+
z=1)、0.10≦m≦0.40の範囲のものであるこ
とが分つた。
次に本発明の準垂直磁化膜をもつ試料の記録再
生特性を測定した。比較のため、完全な垂直磁化
膜をもつ試料と完全な斜め蒸着磁化膜をもつ試料
につき測定した。膜厚は全て2000Åの一定とし
た。その結果を下記表に示す。
The present invention relates to a magnetic recording medium suitable for recording using a ring head, a method for manufacturing the same, and an apparatus for manufacturing the same. When a conventional magnetic recording medium with a perpendicular magnetization film is used for recording with a ring head, the ring head generates a semicircular magnetic field as shown in Figure 1, so its high-density recording characteristics are lower than that of a perpendicular head. It has the disadvantage of poor reproduction output. That is, in a ring head, the magnetic field component in the perpendicular direction is strong on the surface side of the perpendicularly magnetized film, but the magnetic field component in the parallel direction is large on the side away from the head, that is, inside the film or near the interface with the substrate. Therefore, the inside of the film and the vicinity of the interface with the substrate are not sufficiently magnetized. this is,
This is because the parallel direction is a difficult magnetization direction in a completely perpendicularly magnetized film. As a result of various studies on this point, the present invention has improved this and has a completely perpendicular magnetization film (Hc⊥/Hc>1,
Mr
A magnetic recording body comprising a quasi-perpendicular magnetization film that satisfies the following conditions on a non-magnetic substrate. Hc⊥/Hc≧1 Hc≧400θe 1≧Mr⊥/Mr≧0.5 where Hc⊥: Coercive force perpendicular to the film surface Hc: Parallel to the film surface in the traveling direction during recording and reproduction Coercive force Mr⊥: Residual magnetization in the direction perpendicular to the film surface Mr: Residual magnetization in the direction parallel to the film surface during recording and reproduction The quasi-perpendicular magnetization of the above magnetic recording body of the present invention using a ring head Figure 2 shows how the film is magnetized.The film a has magnetic anisotropy in the vertical direction and has a large coercive force in the perpendicular direction, so near the film surface where the magnetic field component in the perpendicular direction is large, As in the case of using a conventional completely perpendicularly magnetized film, it is magnetized vertically, and inside the film and near the interface with the substrate b, it is magnetized along the horizontal magnetic field component of the semicircular magnetic field generated by the ring head c. Since it is magnetized, the demagnetizing field inside the film and near the interface with the substrate a2 is reduced, and therefore high reproduction output and high recording density characteristics can be obtained. Thus, the quasi-perpendicularly magnetized film of the present invention can be magnetized along the magnetic field generated by the ring head. In particular, a large demagnetizing field is generated in the perpendicular direction on the film surface, so Hc⊥/
The condition that Hc>1 is essential. In addition to the above magnetic properties, if the direction of magnetic anisotropy in the film plane matches the recording direction, the self-demagnetizing effect can be further reduced, further improving high-density recording properties and reproduction output. be able to. In the case of a magnetic tape, this direction is the longitudinal direction, and in the case of a disk, it is the circumferential direction. In this quasi-perpendicularly magnetized film, the magnetic anisotropy of the entire film is in the perpendicular direction, as can be seen from the above characteristic conditions, and furthermore, the magnetic property is that the anisotropy on the film surface coincides with the recording direction. It's summery. First,
The inventors created a (Fe, Co, Ni)-O-based perpendicularly magnetized film by depositing Fe, Co, Ni, or their alloys on a non-heated non-magnetic substrate surface in a vacuum atmosphere with O 2 gas introduced. Although a method of manufacturing by almost perpendicular incident deposition has been proposed, it has been found that the above-mentioned quasi-perpendicularly magnetized film can be manufactured by a method substantially similar to this method. That is, in the above manufacturing method, it is sufficient to reduce the perpendicular magnetism to some extent,
For example, it has been found that it can be obtained by performing similar almost vertical deposition on a nonmagnetic substrate heated and maintained at a temperature in the range of 100 to 400°C. In other words, when a mixture of non-ferromagnetic oxide particles and metal ferromagnetic particles adheres to a heated substrate, the heat causes the metal ferromagnetic particles to become coarser, increasing the coercive force and at the same time disrupting the vertical alignment. It has been found that the magnetic anisotropy is reduced, resulting in a quasi-perpendicularly magnetized film of the present invention. When the temperature significantly exceeds 400°C, the coercive force decreases because the particle size becomes too large. The quasi-perpendicular magnetization film can be manufactured by any of the vacuum evaporation method, ion plating method, and sputtering method. Next, an embodiment of the method of manufacturing a magnetic recording medium having the quasi-perpendicular magnetization film according to the present invention will be described in detail with reference to FIG. 3, together with a typical manufacturing apparatus. Reference numeral 1 denotes a vacuum processing container having an exhaust port 2 connected to a vacuum pump. Inside the container 1, a heated rotating metallic cylinder 3 is placed at the center, and a tape-shaped non-magnetic material is placed on both sides above the container. An unwinding roller 4 and a winding roller 5 are provided for the base material a, and the tape-shaped non-magnetic base material b is spanned between these 4 and 5 with it being attached to the circumferential surface of the cylindrical body 3 in the middle thereof, This was made to run at a predetermined speed in the direction of the arrow. An electron beam evaporation source 6 is provided directly below the cylindrical body 3, a small gap 7 is provided near the lower end surface of the cylindrical body 3, and adhesion prevention plates 8 and 9 are provided on both sides of the gap 7. One deposition prevention plate A is installed horizontally so that it can be moved left and right in the drawing, and the evaporated atoms of material B made of Fe, Co, Ni, or alloys thereof from the evaporation source 6 are deposited at an incident angle of θ 1 . It is now possible to adjust the settings as appropriate. The angle of incidence θ 2 with respect to one of the adhesion prevention plates 9 can also be made freely movable as required. Further, an O 2 introduction pipe 10 that opens into the evaporation region so that O 2 can be blown out is provided to penetrate the wall of the container 1 in an airtight manner. Use such a device and operate it as follows. That is, the non-magnetic substrate a 2 is moved in the direction of the arrow and brought into contact with the outer peripheral surface of the cylindrical body 3 which has been heated from the inside to, for example, 300°C by any means, and the substrate b is heated to 300°C. , ferromagnetic metal evaporated atoms rising from below through the gap 7 are deposited on the surface a of the heating substrate at an almost perpendicular incidence angle while passing through the lower end surface of the cylindrical body 3, and the quasi-perpendicularly magnetized film a After it is formed, it is wound up on the roller 5. As a comparison test, θ 1 was set to 0° and 30°.
We talked about types. θ 2 was kept constant at 30°. In-plane magnetic anisotropy of the created magnetized film is not observed when θ 1 is 0°, but when θ 1 is 30°, in-plane magnetic anisotropy occurs in the longitudinal direction of the tape. did. This is because the direction of the nucleus that initially appears on the base material surface determines the direction of subsequent crystal growth; when θ 1 is 0°, the crystal grows vertically, but when θ 1 is 30°, the crystal grows vertically. This is considered to be because crystal growth occurs with a slight inclination in the longitudinal direction in the case of .degree. On the other hand, due to the heat of the heated base material, the particles become coarser and their vertical alignment is disrupted, thereby ensuring the production of the quasi-perpendicularly magnetized film of the present invention. Using the above apparatus, various compositions of Fe, Co, Ni, and their alloys, and these various metals and O
We created various magnetized films with different compositions of atoms and measured their various magnetic properties. The results are shown in FIGS. 4 to 15. From these results, it can be seen that the quasi-perpendicularly magnetized film of the present invention having the above magnetic property conditions is (Fe x Co y
Ni z ) 1-n On the composition represented by n , 0≦x≦
0.05, 0≦z≦0.40 (x+y+z=1), 0.10
In the range of ≦m≦0.40 and the above composition, 0.40≦x≦1.0, 0≦z≦0.25 (however, x+y+
z=1), and 0.10≦m≦0.40. Next, the recording and reproducing characteristics of the sample having the quasi-perpendicular magnetization film of the present invention were measured. For comparison, measurements were taken on a sample with a completely perpendicular magnetization film and a sample with a completely obliquely deposited magnetization film. All film thicknesses were kept constant at 2000 Å. The results are shown in the table below.
【表】
茲でHcはテープの長さ方向に測定した面内
保磁力、*Hcは、テープの巾方向に測定した面
内保磁力を示す。試料No.1、3は入射角θ1を0゜に
して作成したもので、試料No.2は、入射角θ1を
30゜にして作成したものでHc(θe)か*Hc(θe)
より大きく、明らかに膜面内における磁気異方性
の方向が記録再生時に走行させる方向と一致して
いる特性をもつ。試料No.4は、Hcの値が300θe
で不適である。試料No.5はMr⊥/Mrが1.5で
完全な垂直磁化膜である。試料No.6はHc⊥/
Hc=0.7で完全な斜め磁化膜である。
これら試料の4分の1インチ幅の磁気テープ
を、オープンリール型オーデイオデツキを改造し
た測定器を用いて再生出力を測定した。測定時の
テープ走行速度は4.8cm/secとした。記録は正弦
波を用いた夫々の周波数において最適記録電流を
求めて行なつた。その結果を第16図に示す。こ
の図から、本発明品試料No.1〜3において優れた
記録再生特性が得られることが分る。このように
本発明によるときは、非磁性基板上に、Hc⊥/
Hc≧1、Hc≧400θe、1≧MC⊥/Mc≧
0.5の磁気特性をもつ準垂直磁化膜をもつ磁気記
録体とすることにより、リングヘツドに適用し高
密度記録並に高再生出力が得られ、又その製造
は、非磁性基板を加熱した状態でFe、Co、Ni又
はその合金の原子を酸素の導入下で該基板に蒸着
するようにしたので、前記特定の条件の(Fe、
Co、Ni)−O系の準垂直磁化膜を確実に高能率に
得られる効果を有する。[Table] Hc indicates the in-plane coercive force measured in the length direction of the tape, * Hc indicates the in-plane coercive force measured in the width direction of the tape. Samples No. 1 and 3 were created with the incident angle θ 1 set to 0°, and sample No. 2 was created with the incident angle θ 1 set to 0°.
Hc (θe) or * Hc (θe) for the one created at 30°
It has a characteristic that the direction of magnetic anisotropy within the film plane clearly matches the direction in which it travels during recording and reproduction. Sample No. 4 has an Hc value of 300θe
It is inappropriate. Sample No. 5 has Mr⊥/Mr of 1.5 and is a perfectly perpendicularly magnetized film. Sample No. 6 is Hc⊥/
With Hc=0.7, it is a perfectly diagonally magnetized film. The playback output of these sample magnetic tapes having a width of 1/4 inch was measured using a measuring device modified from a reel-to-reel audio deck. The tape running speed during measurement was 4.8 cm/sec. Recording was performed using a sine wave to determine the optimum recording current at each frequency. The results are shown in FIG. From this figure, it can be seen that excellent recording and reproducing characteristics are obtained in the invention sample Nos. 1 to 3. In this way, according to the present invention, Hc⊥/
Hc≧1, Hc≧400θe, 1≧MC⊥/Mc≧
By creating a magnetic recording medium with a quasi-perpendicular magnetization film with a magnetic property of 0.5, it is possible to apply it to a ring head and obtain high reproduction output as well as high-density recording. , Co, Ni, or their alloys are deposited on the substrate under the introduction of oxygen.
This has the effect of reliably obtaining a quasi-perpendicular magnetization film based on Co, Ni)-O with high efficiency.
第1図はリングヘツドによる垂直磁化膜に対す
る作動状態の側面図、第2図はリングヘツドによ
る本発明の準垂直磁化膜に対する作動状態の模写
図、第3図は本発明の磁気記録体の製造装置の1
例の正面図、第4図乃至第15図は本発明の
(Fe、Co、Ni)O系組成の準垂直磁化膜の磁気
特性図、第16図は、各試料の再生出力特性図を
示す。
a……準垂直磁化膜、b……基板、1……真空
処理容器、3……加熱される回転円胴体、4,5
……ローラー、6……蒸発源、7……空隙、8,
9……防着板、θ1,θ2……入射角、10……O2導
入管。
FIG. 1 is a side view of the operating state of the ring head on the perpendicularly magnetized film, FIG. 2 is a schematic diagram of the operating state of the ring head on the quasi-perpendicular magnetized film of the present invention, and FIG. 3 is a diagram of the apparatus for producing a magnetic recording medium of the present invention. 1
The front view of the example, FIGS. 4 to 15 are magnetic characteristic diagrams of the quasi-perpendicular magnetization film with the (Fe, Co, Ni)O system composition of the present invention, and FIG. 16 is the reproduction output characteristic diagram of each sample. . a... Quasi-perpendicular magnetization film, b... Substrate, 1... Vacuum processing container, 3... Rotating circular body to be heated, 4, 5
...Roller, 6...Evaporation source, 7...Gap, 8,
9... Anti-adhesion plate, θ 1 , θ 2 ... Incident angle, 10... O 2 introduction pipe.
Claims (1)
準垂直磁化膜を備えることを特徴とする磁気記録
体。 Hc⊥/Hc≧1 Hc≧400θe 1≧Mr⊥/Mr≧0.5 茲で、 Hc⊥:膜面に対して垂直方向の保磁力 Hc:膜面に対して平行方向で記録再生時の走
行方向の保磁力 Mr⊥:膜面に対して垂直方向の残留磁化 Mr:膜面に対して平行方向で記録再生時の走
行方向の残留磁化 2 該準垂直磁化膜は、(FexCoyNiz)1-nOnで表
わされる組成において、0≦x≦0.05、0≦z≦
0.40(但しx+y+z=1)0.10≦m≦0.40の範囲
である特許請求の範囲1に記載の磁気記録体。 3 該準垂直磁化膜は、(FexCoyNiz)1-nOnで表
わされる組成において、0.40≦x≦1.0、0≦z
≦0.25(但しx+y+z=1)、0.10≦m≦0.40の
範囲にある特許請求の範囲1に記載の磁気記録
体。 4 該準垂直磁化膜は、膜面内における磁気異方
性の方向が記録再生時に走行させる方向と一致し
ている特許請求の範囲1に記載の磁気記録体。 5 非磁性基板を約100〜400℃の範囲に加熱した
状態で、これに対し殆んど垂直にFe、Co、Ni原
子又はその合金の磁性金属原子のいづれか1種又
はその複数種を蒸発させると同時にO2ガスを導
入しその準垂直磁化膜を形成することを特徴とす
る磁気記録体の製造法。 6 該準垂直磁化膜は、(FexCoyNiz)1-nOnで表
わされる組成において、0≦x≦0.05、0≦z≦
0.40、(但しx+y+z=1)、0.10≦m≦0.40の
範囲である特許請求の範囲5に記載の製造法。 7 該準垂直磁化膜は、(FexCoyNiz)1-nOnで表
わされる組成において、0.40≦x≦1.0、0≦z
≦0.25(但しx+y+z=1)、0.10≦m≦0.40の
範囲である特許請求の範囲5に記載の製造法。 8 その磁性金属原子を加熱基板に対しθ1≧0で
蒸着する特許請求の範囲5に記載の製造法。 9 真空処理容器内に非磁性基材を添着すべき加
熱される円胴体とその直下に蒸発源を設けると共
にその円胴体の下端面近傍に空隙を存してその両
側に防着板を設け、更に真空容器にO2導入孔を
設けて成る磁気記録体の製造装置。[Claims] 1. A magnetic recording body comprising a quasi-perpendicular magnetization film that satisfies the following conditions on a non-magnetic substrate. Hc⊥/Hc≧1 Hc≧400θe 1≧Mr⊥/Mr≧0.5 where Hc⊥: Coercive force perpendicular to the film surface Hc: Parallel to the film surface in the traveling direction during recording and reproduction Coercive force Mr⊥: Residual magnetization in the direction perpendicular to the film surface Mr: Residual magnetization in the direction parallel to the film surface and in the running direction during recording and reproduction 2 The quasi-perpendicularly magnetized film is (F x Co y Ni z ) In the composition represented by 1-n O n , 0≦x≦0.05, 0≦z≦
0.40 (where x+y+z=1) 0.10≦m≦0.40, the magnetic recording body according to claim 1. 3 The quasi-perpendicularly magnetized film has a composition represented by (F x Co y Ni z ) 1-n O n , 0.40≦x≦1.0, 0≦z
The magnetic recording body according to claim 1, which is in the range of ≦0.25 (where x+y+z=1) and 0.10≦m≦0.40. 4. The magnetic recording body according to claim 1, wherein the quasi-perpendicularly magnetized film has a direction of magnetic anisotropy in the film plane that coincides with a direction in which the film travels during recording and reproduction. 5. While heating the nonmagnetic substrate to a temperature in the range of approximately 100 to 400°C, evaporate one or more magnetic metal atoms such as Fe, Co, Ni atoms, or their alloys almost perpendicularly to the nonmagnetic substrate. A method for producing a magnetic recording material, characterized by simultaneously introducing O 2 gas and forming a quasi-perpendicular magnetization film. 6 The quasi-perpendicularly magnetized film has a composition represented by (F x Co y Ni z ) 1-n O n such that 0≦x≦0.05, 0≦z≦
0.40, (where x+y+z=1), 0.10≦m≦0.40, the manufacturing method according to claim 5. 7 The quasi-perpendicularly magnetized film has a composition represented by (Fe x Co y Ni z ) 1-n O n , 0.40≦x≦1.0, 0≦z
The manufacturing method according to claim 5, wherein the range is ≦0.25 (where x+y+z=1) and 0.10≦m≦0.40. 8. The manufacturing method according to claim 5, wherein the magnetic metal atoms are deposited on the heated substrate at θ 1 ≧0. 9 A heated cylindrical body to which a non-magnetic base material is to be attached is provided in a vacuum processing container, an evaporation source is provided directly below the evaporation source, and a gap is provided near the lower end surface of the cylindrical body, and adhesion prevention plates are provided on both sides of the cylindrical body. The apparatus for manufacturing a magnetic recording medium further includes an O 2 introduction hole provided in the vacuum container.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4933084A JPH0248966B2 (en) | 1984-03-16 | 1984-03-16 | JIKIKIROKUTAI * SONOSEIZOHONARABINISEIZOSOCHI |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4933084A JPH0248966B2 (en) | 1984-03-16 | 1984-03-16 | JIKIKIROKUTAI * SONOSEIZOHONARABINISEIZOSOCHI |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60195736A JPS60195736A (en) | 1985-10-04 |
| JPH0248966B2 true JPH0248966B2 (en) | 1990-10-26 |
Family
ID=12827974
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP4933084A Expired - Lifetime JPH0248966B2 (en) | 1984-03-16 | 1984-03-16 | JIKIKIROKUTAI * SONOSEIZOHONARABINISEIZOSOCHI |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0248966B2 (en) |
-
1984
- 1984-03-16 JP JP4933084A patent/JPH0248966B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS60195736A (en) | 1985-10-04 |
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